利用W波段高T_c超导-介质谐振器测量YBa_2Cu_3O_(7-x)薄片的毫米波表面阻抗

本文报道利用高 T_c 超导-介质谐振器测量 YBa_2Cu_3O(7-x)表面阻抗随温度的变化.谐振器由蓝宝石管两端加载 YBCO 超导片组成.测量表明,当温度渐降低于80K 时,样品的表面电阻 R_s 迅速下跌;但在低的相对温度下(如t=0.2=T/T_c),样品的 R_s 仍较大,与 BCS 理论预计相去甚远.文中还提出决定λ_L(t)的一种新方法,并从我们的实测数据导出最佳拟合曲线满足λ_L(t)=λ_L(0)(1-t~2)~(-1/2).     

反铁磁材料中的空间磁孤子和非线性磁波的传播

给出了反铁磁材料(anti-ferromagnet)对圆偏报电磁波响应的非线性磁化率显式,由此导出了磁波满足的非线性波动方程。从理论上揭示了在反铁磁材料中传播的非线性线偏振磁波波束在其稳态和非稳态情况下都以空间孤子的形式存在,其空间宽度与自身的频率有关,当与频率有关的非线性磁化率为负值时,平面磁波才具有传播稳定性。     

铁磁薄膜中非线性静磁表面波的传播

本文用微扰理论导出了横向磁化条件下铁磁薄膜中非线性静磁表面波满足的运动方程和它的解析解。获得非线性色散关系,揭示了传播功率致使静磁表面波频带压缩。研究了群色散和非线性频移随频率和薄膜厚度的变化规律。证明了横向磁化时非线性MSSW不能以静磁孤子的形式存在。 关键词：     

YBa_2Cu_3O_(7-δ)超导体的微波特性

本文对YBa_2Cu-3O_(7-δ)材料的表面阻抗的系列研究工作进行了归纳.与经典超导体相比,该类氧化物超导体的微波表面电阻在低温区所呈现的反常,当源于材料的内在特性.我们认为它是材料中存在一定量的未配对载流子所致;而其中 CuO 链的影响是应当考虑的.基于YBa_2Cu_3O_(7-δ)的格胞排序组构,借鉴 Allender 模型,我们提出了修正电导率σ.∝ln(Δ/(?)ω)·[c_1e~(-Δ/K_BT)+(1-c_1)((K_BT)/Δ)]来表征材料的传导电性.基于该设想的微波表面阻抗理论值能很好地吻合实验数据;进而,据此可估计出 YBa_2Cu_3O_(7-δ)的序参数值.如 H_c_1H_c_2,ξ,Δ(0),l.     

利用W波段高T_c超导-介质谐振器测量YBa_2Cu_3O_(7-x)薄片的毫米波表面阻抗

本文报道利用高 T_c 超导-介质谐振器测量 YBa_2Cu_3O(7-x)表面阻抗随温度的变化.谐振器由蓝宝石管两端加载 YBCO 超导片组成.测量表明,当温度渐降低于80K 时,样品的表面电阻 R_s 迅速下跌;但在低的相对温度下(如t=0.2=T/T_c),样品的 R_s 仍较大,与 BCS 理论预计相去甚远.文中还提出决定λ_L(t)的一种新方法,并从我们的实测数据导出最佳拟合曲线满足λ_L(t)=λ_L(0)(1-t^2)^(-1/2).     

反铁磁晶体中的非线性TE表面波

将反铁磁晶体中ＴＥ表面波满足的非线性波动方程变形为伯努利微分方程，用反函数形式给出了表面波磁场的精确解．证明非线性ＴＥ表面波存在的必要条件是μ_x＞０．求得了色散方程，分析了非线性ＴＥ波的频率范围．理论结果表明，导波磁场峰值位置具有稳定性，同功率无关；在ε₁＞ε₂条件下，在功率阈值之上，一个传播功率对应两个不同的有效折射率，表面导波具有双稳特性 关键词：     

PHOTON ACCELERATION DRIVEN BY AN INTENSE LASER PULSE

Interaction of a laser field with a plasma wave is studied by metric optics. Analysis shows that the frequency upshifting of the laser pulse results from the plasma density gradient. A laser beam can be thought of as a packet of photons moving in a plasma and thus the laser frequency upshifting is equivalent to photon acceleration. Examination of the three-dimensional motion equations shows that a laser beam diffraction occurs in the presence of a radial variation of the plasma density. It is argued that the focusing mechanism originating from the plasma wave can curb laser diffraction so that photons may be trapped in the plasma wave and accelerated continuously.     

NON-EQUILIBRIUM MICROWAVE RESPONSE OF Yba2Cu3O7-δ GRANULAR THIN FILMS UNDER MAGNETIC FIELDS

Microwave responses of YBa₂Cu₃O_7-δ(YBCO) granular film have been studied at the microwave frequency of 30.5 GHz. In the absence of a magnetic field the dependence of a normal microwave response on the bias current is observed at a temperature close to T_c. When a magnetic field ranged from 5.0 mT to 33.0 mT is applied, the responses broaden and shift toward a lower temperature. In the superconducting state, the responses were found to be highly dependent on the magnetic field. For the current equal to 5.0mA and a magnetic field above 17.0mT the response increases and did not vanish even at a very low temperature, the fact is believed to be correlated to the anisotropic character of the structure.     

NON-EQUILIBRIUM MICROWAVE RESPONSE OF Yba2Cu3O7-δ GRANULAR THIN FILMS UNDER MAGNETIC FIELDS

Microwave responses of YBa₂Cu₃O_7-δ(YBCO) granular film have been studied at the microwave frequency of 30.5 GHz. In the absence of a magnetic field the dependence of a normal microwave response on the bias current is observed at a temperature close to T_c. When a magnetic field ranged from 5.0 mT to 33.0 mT is applied, the responses broaden and shift toward a lower temperature. In the superconducting state, the responses were found to be highly dependent on the magnetic field. For the current equal to 5.0mA and a magnetic field above 17.0mT the response increases and did not vanish even at a very low temperature, the fact is believed to be correlated to the anisotropic character of the structure.